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Uniform closeness of large circles of fast planes to the asymptotic orbit

Proved
FiniteEnergyPlane.exists_loop_near_orbit_of_mem_fastPlaneSet

by Mazecto · Nov 4, 2026 · Mathlib 0df444a (Lean v4.33.1)

compactnesspseudoholomorphic-curvesreeb-dynamicssymplectization

Let P=(x,T)P=(x,T)P=(x,T) be a periodic Reeb orbit on a strictly star-shaped level S⊂R4S\subset\mathbb{R}^4S⊂R4 such that every periodic orbit of period at most TTT is nondegenerate, and let 0<γ0<\gamma0<γ be smaller than every such period and every difference of two distinct such periods. For every ε>0\varepsilon>0ε>0 there is a radius ρ0\rho_0ρ0​ such that, for every plane uuu in the set Θ(K,P)\Theta(K,P)Θ(K,P) of fast finite-energy planes asymptotic to PPP at ∞\infty∞ with u(0)∈Ku(0)\in Ku(0)∈K and dλd\lambdadλ-energy γ\gammaγ outside the closed unit disk, and every ρ≥ρ0\rho\ge\rho_0ρ≥ρ0​, the loop t↦pr(u(ρe2πit))t\mapsto\mathrm{pr}(u(\rho e^{2\pi it}))t↦pr(u(ρe2πit)) is uniformly ε\varepsilonε-close to t↦x(Tt+c)t\mapsto x(Tt+c)t↦x(Tt+c) for some phase ccc.

The radius does not depend on uuu or on KKK. This is the uniform control at ∞\infty∞ used for sequences of such planes.

Formalization Note R4∖{0}≅R×S\mathbb{R}^4\setminus\{0\}\cong\mathbb{R}\times SR4∖{0}≅R×S is V 1 \ {0}, with aaa = aCoord H and pr\mathrm{pr}pr = proj H; Θ\ThetaΘ = fastPlaneSet H J P K γ. The loop is loopInS H u (ccwLoop ρ). The phase ccc may depend on uuu and ρ\rhoρ.

Preamble
import Definitions.Def_FiniteEnergyPlane_Compactness
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Let `P` be a periodic Reeb orbit on `S ⊂ ℝ⁴` such that every periodic orbit of period at most
`P.T` is nondegenerate, and let `0 < γ` be smaller than every such period and every difference of two
distinct such periods. For every `ε > 0` there is a radius `ρ₀`, independent of the plane, such that
for every `u ∈ fastPlaneSet H J P K γ` and every `ρ ≥ ρ₀` the loop `t ↦ proj(u(ρ e^{2πit}))` is
uniformly `ε`-close to `t ↦ P.x(P.T t + c)` for some phase `c`. -/
theorem exists_loop_near_orbit_of_mem_fastPlaneSet (H : V 1 → ℝ) (hH : IsStrictlyStarShapedLevel H)
    (J : V 1 → V 1 →L[ℝ] V 1) (hJ : IsCompatibleXiStructure H J) (P : ReebOrbit H)
    (hnd : ∀ Q : ReebOrbit H, Q.T ≤ P.T → Q.IsNondegenerate)
    (γ : ℝ) (hγ : 0 < γ) (hγ₁ : ∀ Q : ReebOrbit H, Q.T ≤ P.T → γ < Q.T)
    (hγ₂ : ∀ Q₁ Q₂ : ReebOrbit H, Q₁.T ≤ P.T → Q₂.T ≤ P.T → Q₁.T ≠ Q₂.T → γ < |Q₁.T - Q₂.T|)
    (K : Set (V 1)) (ε : ℝ) (hε : 0 < ε) :
    ∃ ρ₀ : ℝ, 0 < ρ₀ ∧ ∀ u ∈ fastPlaneSet H J P K γ, ∀ ρ : ℝ, ρ₀ ≤ ρ →
      ∃ c : ℝ, ∀ t : ℝ, ‖loopInS H u (ccwLoop ρ) t - P.x (P.T * t + c)‖ ≤ ε := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, Trans. AMS 364 (2012), arXiv:0812.4076, Section 4 (Lemma 4.17 and its proof)

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